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Chapter 25 Reflection and Refraction of Light Fig. 25-CO,2p. 839 25.1 The Nature of Light Before the beginning of the nineteenth century, light was considered to be a stream of particles The particles were emitted by the object being viewed, Newton was the chief architect of the particle theory of light He believed the particles left the object and stimulated the sense of sight upon entering the eyes 3 Nature of Light – Alternative View Christian Huygens argued the light might be some sort of a wave motion Thomas Young (1801) provided the first clear demonstration of the wave nature of light He showed that light rays interfere with each other Such behavior could not be explained by particles 4 More Confirmation of Wave Nature During the nineteenth century, other developments led to the general acceptance of the wave theory of light Maxwell asserted that light was a form of high-frequency electromagnetic wave Hertz confirmed Maxwell’s predictions 5 Particle Nature Some experiments could not be explained by the wave nature of light The photoelectric effect was a major phenomenon not explained by waves When light strikes a metal surface, electrons are sometimes ejected from the surface The kinetic energy of the ejected electron is independent of the frequency of the light 6 Dual Nature of Light In view of these developments, light must be regarded as having a dual nature In some cases, light acts like a wave, and in others, it acts like a particle 7 The Ray Approximation in Geometric Optics Geometric optics involves the study of the propagation of light The ray approximation is used to represent beams of light A ray is a straight line drawn along the direction of propagation of a single wave It shows the path of the wave as it travels through space It is a simplification model 8 Ray Approximation The rays are straight lines perpendicular to the wave fronts With the ray approximation, we assume that a wave moving through a medium travels in a straight line in the direction of its rays Fig 25.1 9 Ray Approximation at a Barrier A wave meets a barrier with l<<d d is the diameter of the opening The individual waves emerging from the opening continue to move in a straight line This is the assumption of the ray approximation Good for the study of mirrors, lenses, prisms, and associated optical instruments Fig 25.2(a) 10 Ray Approximation at a Barrier, cont The wave meets a barrier whose size of the opening is on the order of the wavelength, l~d The waves spread out from the opening in all directions The waves undergo diffraction Fig 25.2(b) 11 Ray Approximation at a Barrier, final The wave meets a barrier whose size of the opening is much smaller than the wavelength l >> d The diffraction is so great that the opening can be approximated as a point source Fig 25.2(c) 12 Active Figure 25.2 • If you can't see the image above, please install Shockwave Flash Player. • If this active figure can’t auto-play, please click right button, then click play. NEXT 13 Reflection of Light A ray of light, the incident ray, travels in a medium When it encounters a boundary with a second medium, part of the incident ray is reflected back into the first medium This means it is directed backward into the first medium 14 Specular Reflection Specular reflection is reflection from a smooth surface The reflected rays are parallel to each other All reflection in your text is assumed to be specular Fig 25.4(a) 15 Diffuse Reflection Diffuse reflection is reflection from a rough surface The reflected rays travel in a variety of directions A surface behaves as a smooth surface as long as the surface variations are much smaller than the wavelength of the light Fig 25.4(b) 16 Law of Reflection The normal is a line perpendicular to the surface It is at the point where the incident ray strikes the surface The incident ray makes an angle of θ1 with the normal The reflected ray makes an angle of θ1' with the normal Fig 25.5 17 Active Figure 25.5 • If you can't see the image above, please install Shockwave Flash Player. • If this active figure can’t auto-play, please click right button, then click play. NEXT 18 Law of Reflection, cont The angle of reflection is equal to the angle of incidence θ1'= θ1 This relationship is called the Law of Reflection The incident ray, the reflected ray and the normal are all in the same plane 19 20p. 844 Fig. 25-6a, 21p. 844 Fig. 25-6b, Multiple Reflections The incident ray strikes the first mirror The reflected ray is directed toward the second mirror There is a second reflection from the second mirror Apply the Law of Reflection and some geometry to determine information about the rays Fig 25.7 22 Some Additional Points The path of a light ray is reversible This property is useful for geometric constructions Applications of the Law of Reflection include digital projection of movies, TV shows and computer presentations Using a digital micromirror device Contains more than a million tiny mirrors that can be individually tilted and each corresponds to a pixel in the image 23 24 25 26 25.4 Refraction of Light When a ray of light traveling through a transparent medium encounters a boundary leading into another transparent medium, part of the energy is reflected and part enters the second medium The ray that enters the second medium is bent at the boundary This bending of the ray is called refraction 27 Refraction, 2 The incident ray, the reflected ray, the refracted ray, and the normal all lie on the same plane The angle of refraction depends upon the material and the angle of incidence sin 1 v 2 constant sin 2 v1 v1 is the speed of the light in the first medium and v2 is its speed in the second medium 28 Refraction of Light, 3 The path of the light through the refracting surface is reversible For example, a ray travels from A to B If the ray originated at B, it would follow the line AB to reach point A Fig 25.8 29 Following the Reflected and Refracted Rays Ray is the incident ray Ray is the reflected ray Ray is refracted into the lucite Ray is internally reflected in the lucite Ray is refracted as it enters the air from the lucite Fig 25.8 30 Active Figure 25.8 • If you can't see the image above, please install Shockwave Flash Player. • If this active figure can’t auto-play, please click right button, then click play. NEXT 31 25.4 Refraction Details, 1 Light may refract into a material where its speed is lower The angle of refraction is less than the angle of incidence The ray bends toward the normal Fig 25.9 32 Refraction Details, 2 Light may refract into a material where its speed is higher The angle of refraction is greater than the angle of incidence The ray bends away from the normal Fig 25.9 33 Active Figure 25.9 • If you can't see the image above, please install Shockwave Flash Player. • If this active figure can’t auto-play, please click right button, then click play. NEXT 34 Light in a Medium The light enters from the left The light may encounter an atom, as in A The atom may absorb the light, oscillate, and reradiate the light This can repeat at atom B The absorption and radiation cause the average speed of the light moving through the material to decrease Fig 25.10 35 The Index of Refraction The speed of light is a maximum in a vacuum The index of refraction, n, of a medium can be defined as speed of light in a vacuum n average speed of light in a medium c n v 36 Index of Refraction, cont For a vacuum, n = 1 We assume n = 1 for air, also For other media, n > 1 n is a dimensionless number greater than unity n is not necessarily an integer 37 Some Indices of Refraction 38 Frequency Between Media As light travels from one medium to another, its frequency does not change Both the wave speed and the wavelength do change The wavefronts do not pile up, nor are created or destroyed at the boundary, so ƒ must stay the same Fig 25.11 39 Index of Refraction Extended The frequency stays the same as the wave travels from one medium to the other v=ƒλ ƒ1 = ƒ2 but v1 v2 so l1 l2 The ratio of the indices of refraction of the two media can be expressed as various ratios c l1 v1 n1 n2 l2 v 2 c n1 n2 40 More About Index of Refraction The previous relationship can be simplified to compare wavelengths and indices: l1 n1 = l2 n2 In air, n1 1 and the index of refraction of the material can be defined in terms of the wavelengths l l in vacuum n ln l in material 41 Snell’s Law of Refraction n1 sin θ1 = n2 sin θ2 θ1 is the angle of incidence θ2 is the angle of refraction The experimental discovery of this relationship is usually credited to Willebrord Snell and therefore known as Snell’s Law 42 25.5 Dispersion For a given material, the index of refraction varies with the wavelength of the light passing through the material This dependence of n on λ is called dispersion Snell’s Law indicates light of different wavelengths is bent at different angles when incident on a refracting material 43 44 45 46 47 48 49 50 51 52 53 Variation of Index of Refraction with Wavelength The index of refraction for a material generally decreases with increasing wavelength Violet light bends more than red light when passing into a refracting material Fig 25.13 54 Angle of Deviation The ray emerges refracted from its original direction of travel by an angle d, called the angle of deviation d depends on F and the index of refraction of the material Fig 25.14 55 Refraction in a Prism Since all the colors have different angles of deviation, white light will spread out into a spectrum Violet deviates the most Red deviates the least The remaining colors are in between Fig 25.15 56 The Rainbow A ray of light strikes a drop of water in the atmosphere It undergoes both reflection and refraction First refraction at the front of the drop Violet light will deviate the most Red light will deviate the least 57 The Rainbow, 2 At the back surface the light is reflected It is refracted again as it returns to the front surface and moves into the air The rays leave the drop at various angles The angle between the white light and the most intense violet ray is 40° The angle between the white light and the most intense red ray is 42° Fig 25.16 58 Active Figure 25.16 • If you can't see the image above, please install Shockwave Flash Player. • If this active figure can’t auto-play, please click right button, then click play. NEXT 59 25.6 Observing the Rainbow Fig 25.17 If a raindrop high in the sky is observed, the red ray is seen A drop lower in the sky would direct violet light to the observer The other colors of the spectra lie in between the red and the violet 60 Double Rainbow The secondary rainbow is fainter than the primary and its colors are reversed The secondary rainbow arises from light that makes two reflections from the interior surface before exiting the raindrop Higher-order rainbows are possible, but their intensity is low 61 Christiaan Huygens 1629 – 1695 Best known for his contributions to the fields of optics and dynamics He considered light to be a kind of vibratory motion, spreading out and producing the sensation of sight when impinging on the eye 62 Huygen’s Principle Huygen assumed that light consists of waves rather than a stream of particles Huygen’s Principle is a geometric construction for determining the position of a new wave at some point based on the knowledge of the wave front that preceded it 63 Huygen’s Principle, cont All points on a given wave front are taken as point sources for the production of spherical secondary waves, called wavelets, which propagate outward through a medium with speeds characteristic of waves in that medium After some time has passed, the new position of the wave front is the surface tangent to the wavelets 64 Huygen’s Construction for a Plane Wave At t = 0, the wave front is indicated by the plane AA’ The points are representative sources for the wavelets After the wavelets have moved a distance cΔt, a new plane BB’ can be drawn tangent to the wavefronts BB’ is parallel to AA’ Fig 25.18 65 Huygen’s Construction for a Spherical Wave The inner arc represents part of the spherical wave The points are representative points where wavelets are propagated The new wavefront is tangent at each point to the wavelet Fig 25.18 66 Huygen’s Principle, Example Waves are generated in a ripple tank Plane waves produced to the left of the slits emerge to the right of the slits as twodimensional circular waves propagating outward At a later time, the tangent of the circular waves remains a straight line Fig 25.19 67 Huygen’s Principle and the Law of Reflection The Law of Reflection can be derived from Huygen’s Principle AB is a wave front of incident light The wave at A sends out a wavelet centered on A toward D The wave at B sends out a wavelet centered on B toward C AD = BC = c Dt Fig 25.20 68 Huygen’s Principle and the Law of Reflection, cont Triangle ABC is congruent to triangle ADC cos g = BC / AC cos g’ = AD / AC Therefore, cos g = cos g’ and gg’ This gives θ1 = θ1’ This is the Law of Reflection Fig 25.20 69 Huygen’s Principle and the Law of Refraction Ray 1 strikes the surface and at a time interval Dt later, ray 2 strikes the surface During this time interval, the wave at A sends out a wavelet, centered at A, toward D Fig 25.21 70 Huygen’s Principle and the Law of Refraction, cont The wave at B sends out a wavelet, centered at B, toward C The two wavelets travel in different media, therefore their radii are different From triangles ABC and ADC, we find BC v1Dt sin1 AC AC and AD v 2 Dt sin 2 AC AC 71 Huygen’s Principle and the Law of Refraction, final The preceding equation can be simplified to sin1 v1 sin 2 v 2 sin1 c n1 n2 But sin 2 c n2 n1 and so n1 sin1 n2 sin 2 This is Snell’s Law of Refraction 72 73 74 75 76 77 78 25.7 Total Internal Reflection A phenomenon called total internal reflection can occur when light is directed from a medium having a given index of refraction toward one having a lower index of refraction 79 Possible Beam Directions Possible directions of the beam are indicated by rays numbered 1 through 5 The refracted rays are bent away from the normal since n1 > n2 Fig 25.22 80 Critical Angle There is a particular angle of incidence that will result in an angle of refraction of 90° This angle of incidence is called the critical angle, C sinC n2 for n1 n2 n1 Fig 25.22 81 Active Figure 25.22 • If you can't see the image above, please install Shockwave Flash Player. • If this active figure can’t auto-play, please click right button, then click play. NEXT 82 Critical Angle, cont For angles of incidence greater than the critical angle, the beam is entirely reflected at the boundary This ray obeys the Law of Reflection at the boundary Total internal reflection occurs only when light is directed from a medium of a given index of refraction toward a medium of lower index of refraction 83 84 85 86 87 25.8 Optical Fibers An application of internal reflection Plastic or glass rods are used to “pipe” light from one place to another Applications include medical use of fiber optic cables for diagnosis and correction of medical problems Telecommunications Fig 25.25 88 Optical Fibers, cont A flexible light pipe is called an optical fiber A bundle of parallel fibers (shown) can be used to construct an optical transmission line 89 Construction of an Optical Fiber The transparent core is surrounded by cladding The cladding has a lower n than the core This allows the light in the core to experience total internal reflection The combination is surrounded by the jacket Fig 25.26 90 Multimode, Stepped Index Fiber Stepped index comes from the discontinuity in n between the core and the cladding Multimode means that light entering the fiber at many angles is transmitted Fig 25.27 91 Multimode, Graded Index Fiber This fiber has a core whose index of refraction is smaller at larger radii from the center The resultant curving reduces transit time and reduces spreading out of the pulse Fig 25.29 92 Optical Fibers, final Optical fibers can transmit about 95% of the input energy over one kilometer Minimization of problems includes using as long a wavelength as possible Much optical fiber communication uses wavelengths of about 1 300 nm. 93 94p. 857 Fig. 25-30,
